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Gas exchange                                                          261

                      After one half-life
                      C       / H  t
                        w
                            e  L k  1/2     0
                       C
                        0
                      Thus,
                           ln(  ) 2   ln(  ) 2        5
                      t 1/2                      . 4  33  10  s =  5.01 d
                           k  L  / H  4 . 2  10  6  5 . 1 /
                      This implies that half of the benzene  has been volatilised after approximately 5 days.


                   14.3  REAERATION

                   In the case of oxygen  exchange between surface water and the atmosphere, the term k /H in
                                                                                      L
                   Equation (14.11) is referred to as the reaeration  constant  k . The mass balance  for exchange
                                                                  r
                   of oxygen between surface water and the atmosphere is then:
                    dDO                                                               (14.13)
                               k r    DO sat   DO
                     dt
                                                                          -3
                   where  DO  = dissolved oxygen concentration in surface water [M L ],  DO  = saturated
                                                                                sat
                                                                         -3
                   (equilibrium) dissolved oxygen concentration in surface water [M L ], and k  = reaeration
                                                                                 r
                            -1
                   constant   [T ]. The saturated dissolved oxygen concentration  DO  depends on the water
                                                                        sat
                   temperature . The following empirical expression is commonly used to determine DO  in mg
                                                                                     sat
                    -1
                   l  as function of temperature (Lijklema, 1991):
                    DO       14 . 652  . 0  41022 T    . 0  007991T  2  . 0  0000777774 T  3  (14.14)
                       sat
                   where T = the water temperature in °C.
                      Oxygen  transfer across the air–water interface is controlled on the water side, because
                   the value of K’  is much larger than 0.01 (see Table 14.1). This means that the overall gas
                               H
                   exchange coefficient  depends on the hydrodynamic characteristics of the air–water interface
                   and the flow regime. The surface renewal model  – an alternative model for gas exchange
                   across the air–water interface – assumes that turbulent eddies bring small parcels of water
                   to the water surface. As long as these parcels are at the surface they can equilibrate with the
                   atmosphere. After equilibrium  is reached, the chemical flux across the air–water interface
                   stops. If fresh parcels replace the depleted parcels more quickly, the flux becomes larger.
                   In deep flowing waters, the renewal rate in the mixing depth near the water surface is
                   approximately equal to the average flow velocity divided by the water depth. This assumption
                   leads to the O’Connor and Dobbins (1958) formula for estimation of the gas exchange
                   coefficient:

                             D  u          u                                          (14.15)
                    k  L      w       3 .90
                              H            H
                                                  -1
                   where u = the average flow velocity (m s ) and H = the water depth (m). The surface renewal
                   model  thus assumes that the gas exchange coefficient  is proportional to the square root of
                   the molecular diffusion  coefficient in water D , in contrast to the thin film model , which
                                                        w
                   assumes that the gas exchange coefficient is proportional to D  (see Equation 14.4). Besides
                                                                    w
                   this theoretically derived Equation (14.15), a number of empirical relationships have been








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